Low energy \(e^+e^-\)  collision experiments, where \(\rho \) , \(\omega \)  and \(\phi \) 
resonances as well as their excited states are produced copiously, offer an ideal
test-bed to thoroughly investigate the properties of these resonances.
Many experimental results regarding these states have been summarized in the
Particle Data Group (PDG) review [1]}.
Still, the properties of some states are still ambiguous.
Notably, the status of the \(\rho (2000)\) , \(\rho (2150)\) , and \(\rho (2270)\) 
states is unclear, due to insufficient experimental information.
The \(\rho (2000)\)  was found in \(p\bar{p}\)  collisions [2]}, [3]}, [4]}, [5]}, [6]},
and it was explained as a radial excitation of the \(\rho (1700)\)  [6]}
or a mixed state with a significant \(^3D_1\)  component [8]}.
The \(\rho (2150)\)  was initially regarded as a \(2^3D_1\) 
state [9]}, but later was considered to be a \(4^3S_1\)  state [10]}, [11]}, [12]}, [13]}, [14]}.
The \(\rho (2270)\)  was first observed in photo-production [15]}
and categorized as a \(3^3D_1\)  state [13]}.
There are no published results
on \(\rho (2000)\)  and \(\rho (2270)\)  from \(e^+e^-\)  collision experiments.
The \(\rho (2150)\)  has been widely studied in \(e^+e^-\) ,
\(p\bar{p}\) , \(s\) -channel \(N\bar{N}\)  and \(\pi p\)  collision experiments,
but inconsistencies in the measured masses and widths make
the \(\rho (2150)\)  more controversial.
